共查询到16条相似文献,搜索用时 62 毫秒
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Ti-IF钢铁素体变形动态再结晶临界应变模型 总被引:6,自引:0,他引:6
用Thermecmaster-Z热模拟试验机试验得出成分为0.006 7%C-0.045 0%Ti的Ti-IF(无间隙原子)钢在变形温度750~900℃和变形速率0.1~40 s-1时的应力-应变曲线,确定了Zener-Holloman参数Z与应变速率.ε和温度T(K)的关系式Z=.εexp(39 507/T),并建立了临界应变εc与原始晶粒尺寸d0和Z参数的临界应变方程εc=2.314 4×10-3×d-0.8003 9×Z0.050。结果表明,在相同变形速率下,850℃变形时动态再结晶最易发生,当变形温度提高至900℃(两相区)时,即使在低变形速率(1 s-1),也不发生动态再结晶。当变形速率大于1 s-1时,Ti-IF钢热加工时不能出现动态再结晶。临界应变预测值与实测值比较,平均误差≤5%。 相似文献
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采用X射线衍射仪分析IF钢铁素体区热轧织构以及退火织构的演化,在实验室热轧机上进行了IF钢的铁素体区热轧,研究了摩擦对IF钢铁素体区热轧、退火织构的影响。结果表明:无润滑轧制时,钢板表层形成强高斯织构组分{110}〈001〉,弱γ纤维织构,导致再结晶织构中高斯组分强度高,γ纤维织构强度低;润滑轧制时,钢板表层高斯织构组分强度降低,{100}〈011〉、γ纤维织构强度提高,退火后γ纤维织构强度提高。钢板中心受摩擦作用影响较小,轧制过程中发展为较强的α和γ纤维织构,退火后γ纤维织构成为主要织构组分。 相似文献
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利用热模拟试验机通过单道次压缩变形试验研究了35K冷墩钢测定奥氏体区形变规律,确定了不同应变率和温度条件下的应力-应变曲线,研究了变形温度、变形速率对试验用钢再结晶行为的影响,建立了35K钢的动态再结晶模型。 相似文献
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采用Gleeble热模拟试验机和透射电镜、扫描电镜及定量金相等分析技术,就钛对低碳Mn-V钢奥氏体晶粒长大行为、奥氏体动态再结晶行为等进行了研究.结果表明,含钛钢中形成稳定的碳氮化钛,对阻止再加热奥氏体晶粒长大有利.含钛钢变形抗力比不含钛钢要高,其动态再结晶开始的临界变形量比不加钛钢的小,易于发生再结晶,且含钛钢的再结晶晶粒尺寸相对较细,再结晶晶粒长大速度也更慢. 相似文献
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低碳钢Q235奥氏体的动态再结晶与动态相变 总被引:2,自引:1,他引:1
对成分为0.18C-0.22Si-0.60Mn(质量分数)的低碳钢在1 100~750 ℃之间的奥氏体动态再结晶及动态相变行为进行了研究.确定了此钢奥氏体发生动态再结晶的临界应变条件及完全动态再结晶后的晶粒尺寸.计算表明,在奥氏体低温区大变形以致使奥氏体发生完全动态再结晶时,可得到6~9 μm 的奥氏体晶粒尺寸.在Ae3以下,变形可以引发动态相变.但奥氏体快速冷却明显推迟了动态相变的发生.与相同温度下单一奥氏体变形相比,有动态相变发生时应力值不增加或降低,其降低程度随变形温度的下降而增加. 相似文献
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Dynamic and Static Recrystallization Behavior of Low Carbon High Niobium Microalloyed Steel 总被引:2,自引:0,他引:2
The recrystallization behavior of a low carbon high Nb microalloyed steel was investigated using Continuous and interrupted hot compression tests. The results showed that the onset of dynamic recrystallization (DRX) could be detected from inflection in the plot of the strain hardening rate θ against stress σ regardless of whether the stress peak appears or not. According to Zener-Hollomon parameter the activity energy of DRX (Qdef) was obtained, and a new modified expression calculating Qdef was proposed in consideration of the chemical composition of experimental steel. Applying the 2% offset method the static softening fraction was determined. The graphic representation of the softening fraction vs. interrupt time gave the information of the non-static recrystallization temperature (about 1000℃)and the relationship of precipitation-time-temperature. Static recrystallization kinetics follow Avrami’s law in high deformation temperature, and different values of the exponent n were given to illustrate the different effects of Nb element on static recrystallization at different deformation temperature. 相似文献
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Hot compression deformation behaviors of medium carbon Cr-Ni-Mo-Nb steel were investigated at deformation temperatures ranging from 1223 to 1423 Kand strain rates of 0.1,1and 5s-1.Dynamic recovery(DRV)and dynamic recrystallization(DRX)were observed during the hot compression deformation.For all of the samples,DRX occurred at deformation temperatures above 1323 Kat different strain rates,while below 1223 K,no DRX was observed.The activation energy of the tested steel was determined as 386.06kJ/mol.The ratio of critical stress to peak stress and the ratio of critical strain to peak strain were 0.835 and 0.37,respectively.Kinetic equations interpreting the DRX behavior of the tested steel were proposed,and the corresponding parameters including the volume fraction and the average grain size were determined.Moreover,the microstructures induced under different deformation conditions were analyzed. 相似文献